Annealing glass



Esc. 18, i956 F. v. ATKESON ANNEALING GLASS Filled May 18, 1953 5 Sheets-Sheet l Dec- 8, i956 F. v. ATKEsoN 2,774,190

ANNEALING GLASS Filed May 18, 1953 5 5 Sheets-Sheet 2 k Fa 2 'isc INVENTOR.

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i8, 1956 F. v. ATKr-:SON 2,7?9399 ANNEALING GLASS Filed May 18, 1955 5 Sheets-Sheet 3 IRESSTANCE HEATERv /AfJ-HEAUNG cmcuvr Bbc-.Hoxe en @f 52-A.c. sommi 56d). C. SOURCE CONTROL comb 6o vARmsLs RsslsToPcSS BY u Dec. 18, 1956 F. v ATKESON ANNEALING GLASS Filed May 18, 1953 5 Sheets-Sheet 4 BGQ \ INVENTOR.

Ame/4N Ll., Kg'so/v Dec. 18, 1956 F. v. ATKESON ANNEALING GLASS 5 Sheets-Sheet 5 Filed May 18, 1953 INNTOR Fide/HIV FIGJ United States Patent O sommaria@ GLASS Florian Y. Atkeson, Springdale, Pa., assignor to Pittsburgh Plate Glass Company, a corporation of Pennsylvania Appneaaon May 1s, 195s, Serin-N0. 355,815

6 Claims. (ci. en -sa) This invention relates in general to the annealing of glass; and more specifically to method of substantially uniform control of the temperature of the cooling glass as it-passes through the annealing range in order to obtain the glass characteristicsdesired. Y

A specific application of the invention isl shown in connection with a conventional window glass vertical drawing machine wherein the glass anneal is improved by controlling a portion of the temperature change in the glass as it moves from the molten state to the finished product in the controlled manner taught by the invention. 'Ihe application of the invention to a horizontally disposed annealing lehr is also taught by a modication of the principal disclosure.

The art of annealing glass is acknowledged to be old and many disclosures are found in the prior art patents of method and apparatus used in attempts to anneal glass under various conditions. Theoretical optimum annealing curves for various glass compositions and shapes are readily calculated but great diificulties have heretofore been encountered in obtaining the desired results. in practice. These ydifficulties have been greatly increased when attempting to obtain the desi-red results i'na window glass drawing machine where precise temperature control is negatived by the necessary structural characteristics of such machines. This isparticuiarly so, due to the necessity for completingthe annealing within a few feet of machine. v A Y The purposeV oftheA improved controll of the rate of cooling of the glass Vsheet or ribbon-during the.` drawing and annealing Ythereof is to produce glass which has a 'minimumA of transverse curvature, optimum optical characteristics resulting from' more uniform thickness of the sheet, a substantially uniform overall residual -stress pattern and improved cutting characteristics.

It has "been found thatl the residual stress' presen-t in annealed glass isv a function or" the time fthe-glass is kept -within=its annealing temperature range and the manner at lleast av minimum period within theV annealingVv range, t

the rate of cooling' the Vglass Yboth above and below the annealing range ld'oes not substantially aiiect: the residual stress Vvalues present in'the annealed glass. It has :been demonstrated that the atness of thel annealed glass. is improved by, reducing the temperature gradients within travel of the glass Vthrough 2,774,190 Patented Dec. 18, 195e ice cools. at. various temperatures and especially, in the annealing range, to provide the annealed glass with an optimum stress for cutting.

It is another object of the present invention to provide an annealing section for use in the manufacture of glass wherein the rate of cooling of the glass is controlled so that the glass isy cooled very rapidly from itsV molten state to av temperature substantially at the `upper limit or top of the annealing temperature range, held at the top of the range for a short time, then cooled slowly but at a-n increasing rate through the range, and then cooled comparatively rapidly below the range, to produce annealed glass having a desirable, residual stress pattern.

Another object Vof the present invention isv to provide window glass having hitherto unobtainable flatness by effective control of temperature gradients across the width and through the thickness of a sheet of window glass being formed in a window glass drawing machine.

Another object of the present invention is to provide a vertical; annealingv section in a drawing machine for use in the manufacture of window glass wherein the rate of draw of the window glass is increasedover the rate presently available,rand simultaneously, wherein a lwindow glass of improved characteristics is made posrate for the glass that conforms as closely as possible to an ideal annealing for obtaining the desired glass characteristics.

Another object of the present invention is to provide a controllable cooling element made up of a series of pipes conveying moving cooling uids and inter-spaced heating elements such that the cooling eiect imparted by the moving tluids may be suitably regulated by controlling the energy input to the heatingelementsv. i Another object of the present invention is to provide within an annealing lehr, a feed back system to 'control the temperature of the glass sheet at any-point Within l the'lehr.. f e

. 'Another object of the present inventionis1 to provide,

in a horizontal or vertical annealing 1ehr,ja system for Y controlling the temperature' ofi-the glass asY itr`passes Va .series of-check points within the l'ehr th-annealingf process to provide a cooling curve for the glass that t conforms as closely as possible to a theoretical cooling curve designed to impart a'desired stress pattern to Vthe Yet another object of the present invention is to pro- V vide an improved method of annealing glass wherein the Stress# values which the glass being drawn, both from edge to edgejandfrom surface to surface, and that the stresses Y.duetotooling the glass being annealed are minimizedfby controlling the .center to surface temperature gradient.l Y

A Primary Obiec't 0f the present inventiontis to amiral glass by improved control of the rate at which the glass ,glass is` rapidly cooled to the upper limit of its annealing n range, its center to- ,surface temperature gradient minimized at that limit and then gradually increased with increasingrapidityA as the glass 'fis cooledk throughy its annealing rangeV to provide the Yannealed glass with an optimum residual stress pattern inthe shortest possible distance`- of travel;

'These and 'other objects of'thefpresentivention Vwill I to the view of Figure 1g' Figurel is a cross-sectional view Vtaken at right angles f Figure 3 is a detailed cross-sectional view of a cooling means utilized to cool the vertically drawn sheet glass rapidly from its molten bath temperature` to the upper region of the annealing range and which forms a novel structural'element in a typical embodiment of the present invention; 'f Y 'i Figure 4 is a chart showing an idealV cooling curve for vertically drawn sheet glass wherein the temperature of the surfaces of the vertically drawnglass sheet isk co1n pared with its vertical'position in a vertically disposed annealing lehr during its upward travel in the lehr;

Figure 5 is a schematic electrical circuit diagram of a typicalelectrical: control circuit useful with the present invention; Y 'Y i Y A l 'Y Figure is aV partly symbolical view( of :portions-of -a horizontal lehr providedV with temperaturefcontrol' ele-r ments for' controlling the temperature Vof a horizontally conveyedV glass sheet as the glass passes through various Y check points within the annealing lehr in accordance with the teaching of the present invention; Y

Figure 7V isV a cross-sectional view ytaken along theV lines 7--7 of Figure Y Y 1 v In order to achieve the objects of the present invention, the cooling of drawn glass isV controlled so that the glass is Vrapidlyanrd uniformly cooled from the molten state to 2,'74,19o i v Y4 its annealing range, 1025 example, between the first pair of drawing rolls 21 and the second pair 22 of a series of paired drawing rolls 21jv ,Y

to 27, inclusive, and to insure a minimum temperature gradient across the width and through the thickness of the v Vglass sheet 10'at thatelevation. Y t

`The heating elements 18 contained in the differential coolers Y are arranged in two sets, generallyrindicated in Figs. l, 3 and'4 as 18 and 18'., of three*independently` controlled circuits. InFig. 2 therthree heating welements 18a, 18h, and lcjofthe circuits ofiset lSar'e shown.

Each of the two setsof. circuits is located torface an op-Y posing surface ofthe rising sheet 10.1.` Each of theheating the upper limitof the-annealingV range and subsequently cooled through its annealing range in such a manner that the glass is properly annealed to the-degree required for elements in 'eacli` of the three independently controlled banks are sandwiched between alternating water cooled 'i elements orpipes.16 which are cooled by continuously Y Y owing water.' Current in .the various heating' elements 18a,v18l 1Y and 18C -isv supplied in response lto thermo-.

responsive control elementsfsuch as thermo-responsive elements 30a, 30b andY 30C, respectively, which are dij rected toward the surface of the glass and supply ther-V mally responsive switching means for the transmission of current through the various heater elements.

Y The thermo-responsive, elements 30. trllzed for this pu'rf pose are aimed at the glass surfacejthrough a 'series ofl sets of portsf29 on each side ofl the glass. The lowermost set of thermo-responsive Velements 30 is sighted on areasV of the 'glass sheet locatedimrnediately below, the' rollers 21 and controls' the current flow in the Vheating:Y

elements of circuits 1S. Y

. By. dividing each horizontal; set of thermo-responsive' elements yinto three independentlycontrolled circuits, the'Y i Y temperature of thev central portion and each end portionff of .the vertically rising sheet Ysurfaces can be independently."V

utilizes a'thermo-responsive-element Atrainedfon larportion of the surface of the rising glass sheet to control the current'ow in a resistance heater by-means of an arrangement that may include a saturable reactor and a feed backV circuit.

, Additionalheatin'g elements'are provided-in theregionV Where the yglass Vtemperature is within the annealing range. The operationof -each additional heatingelementis con` trolledbythe'actionV of a'circuit comprising a temperature l respQIisive switchingmeans, arsaturablereactor anda'feed Y back clrcuit.-Y Eachv temperature responsive. Vnieansizis"V i* trained on a different surface area of vthe plane;-deining the travel of theV glass sheet and is adjusted' to 'provide'the 4range (foneiramplej102521Z), for'adesiredperiod't'o` Y `vision of Yadditional cooling elements with orwithout an y associatediheaterto modify the cooling( eff-ect. `The final' stressfof Wlndowglassso annealed is ,reducedvtoatiprroxi- 'l mately291%V to v50% ofthe stress present inwindow .glass manufacturedby utilizing uncontrolled, machines. :i

Referrrngto-.Figures l, 2 and V3,: whereina ivertical 'accordancelwith 'presentAconventional 'Y Ydrawing methods. 4.immediately above the molten glass bath, ,conventional cooling; means such as` coolers 12',

baby coolers: 13 and waterV cooled catch `pans,14 are provided.

l Vf 'series ofnovel'differential coolers .V15 includingra.V 'Y serles ofwatercooledpipes or tubes 16 af series ,of

heating elements 18 is additionallyV included Ato provide supicient cooling tohavethe vertically drawn sheet-glass reach Va desiredtemperature, namely, that of the 'top' of permitY equalizationV ofv the temperature; of the. .glass throughout its thickness, Yig'lfhen the Vsheet is :cooled through`r i Yand below its annealing range inV conformity withithef'..

,optirnnrn cooling curi/ eras it continues-itsriserA Cooling Y below the annealig .rangeV maybe acceleratedgbythe p1o-' Y The'heat Vimparted Y Y Y trolled byan'independent' electrical c ircuitfrcontaininga thermo-responsive element -thaltgis preset tojsupplyheat; A

controlled Von each' side of ftheV vertically drawn sheet.t

maintains 'a very close Ycontrol of the temperature' of.. the cooling glass The temperature gradient from edge. to edge and from surface to surfaceof'the glass sheet can' Y be kept ati-a minimum'. Also, the height Vabove the'moltenV glassrbath at which theY vertically drawn sheet''reaches a predetermined temperature .correspondingtothe togof j Vtheannealing rangeis regulated.

'H'I'he thermo-responsive elenient'sgfa'rejconstructediwithY i vspecially designed filters, responsive only totheV 4 jto' 8 y mici-on wavelength band ofinfrafred radiation-fl At Wavelength, glassis k(,)paque so'that'th'e thermo-responsive v Velement trained on one fsurface area of the;` glass read's the temperature radiatedbyftheglass surfaceV only and .I Visrnot responsive to heating elements located Ion the other j,

" sideofthe vertically -Adrawn -glassfsheetig'fhe thermo-'1;

responsiveV elements eachVA comprises; a mirror, a; thermopilek at the focal pointn'ofgthei 'mirrongiand' an Y,electric circuit actuatedin responsetoithe.thermopileftqlter Y out radiationQother than.' the desired lfourfto .eightmicron Y 'Wavelength band; VA diensten fype band ,meras-used Y i betwe'enrntheimirrorijand;the .'thermolpilep` Suchidevices lf .A areg'welllkndown in the fartari their rstructuraldetail are" l not part of my invention.A

j Once Vther glass sheetf enters Vthe1annealing.'rangezsoinee wherebetweenfthe first and s econdset-of drawingrolls`,. Y

its temperatureis .controlled by` si3rr additional lrloriz'one VV Y tally aligneclsets ofvr thermo-responsive elements 32,;34, j

, anneallng lehr;is disclosed, a sheet'ofglass 1Q isfdrawn 1;, Y upwardly from a'bathdof moltenglass11 containediinra i responsivefelements hasit's:counterpart.32234236,138;`- 1 40' and-42' reading rtemperatureson;theropposite glass. L surface.: V'TheV Vthern'l-respon'sive. elementsrcontrol fthe amount. of .heating imparted to'ithel'glass at clierentgele- Y f `vatifonsby thelbanks ofhe'ating;e1ernents`'31,*33,735,137fjV 39 Y and z41,-v respectively.` Eachl .bankA of Lheating'elements theris'ing glass'sheet. Y

contains three electrical heaters'f opposite'eachVV surface'l of by *eachl yheating *element*y is -1 con- F., at a desired elevation, for; Y

optimum cutting stress within the -glass for the entire range'of thicknesses produced. l i In practice, as shown in Figure 4, the annealing vintervalis best described as the cross-hatched area 50 under the annealing curve. Area 50a represents the equalizing portion of the annealing interval wherein the lehr temperature is held constant at the top ofthe annealing range in order to minimize the temperature gradient between the center and the surfaces of the rising sheet. Area 50b represents the cooling portion of the annealing curve. Eicacy of annealing is proportional to thetotal area 50 with due consideration for both the preliminary equalizing interval-50a and the shape of the cooling portion 5017.

'In-other words, the amount offresiduallstress that remains in annealed window glass is an inverse function of the time the glass is kept within the optimum annealing temperature range. Furthermore, the time required to obtain an optimum stress pattern in annealed glass increases with the temperature differential existing between the temperature curve through which the glass is :actually annealed and the optimum annealing temperature curve. For commercial purposes, the area 50 as :seen in Fig. 4 should be the maximum possible obtainzable, at least the minimum required for proper anneal, :in the smallest possible time interval.

It is also quite important that there be a minimum wof temperature gradient both across the width and a :minimum of temperature difference for the surfaces of the glass sheet, since the presence of any temperature gradient manifests itself in internal stresses resulting in a distortion of the glass. Thus, in order to obtain at glass, the vminimization of temperature variations at the equalizing ytemperature across the width and through the thickness of the glass sheet is imperative. j

It has been determined that it is unnecessary to maintain the center to surface temperature gradient obtained in the equalization range 56a of Fig.V 4 at a constant 'value during the-subsequent cooling of theglass through the annealing range as shownin areaStlb; kThis discovery enables the glass ribbon'to be controllably cooled through its annealing range whileV theglass istravelling a much shorter distance than'would be necessary to cool' the glass over the same temperature range while maintaining a'constant temperature gradient between the center and the surface of the glass' ribbon; At the same timefvirtually no harmful effectsv such as an increase in stress occur when the center to ysurface gradient is alloWed to increase within controlled limits as the glass `is cooled through its annealing range.

This result is believed to be obtained because the importance of the upper portion of the annealing range in producing residual stress patterns in the glass is greater than the lower portionv of the annealing range due to therapid increase in viscosity of `glass from the upper to the lower limit of the annealing range. This rate of increase is viscosity through the annealing range is an exponential function. For example, in typical plate and window glass vhaving the following chemical compositions, the viscosityin poises at the upper and lower limits of vtheannealing rangeis as follows:

s From the above table, it is evident that the viscosity increases byV a factor of 200 to 300 between the `upper and lower limits of the annealing range. As distortions causing residual stresses are more easily produced in lower .viscosity glass than in glass'of higher viscosity',

'the comparative importance 'of the temperature gradients in the 'glass at the different temperatures Within theanf nealing rangeis apparent. Y Whilev the center to surface gradient obtained in the equalization area of the controlled cooling curve shown in Fig. v4 varies with the thickness of the glass formed, the same principles utilized in controlling the increase in temperaturefgradientrof aV glass of one thickness are necessarily followed in controllably cooling glass of diff ferent thicknesses and compositions through their an; nealing ranges. The following figures are exemplary of a typical glass thickness for drawn window glass. For Window glass l/s" thick having a 50 F. center to surface gradient above the annealing range, the center to surface g-radient is reduced in area V50a to between 2 and 3 F. This gradient is maintained as the glass is slowly cooled through the upper portion of thev annealed range, then gradually increased with increasing rapidity as the temperature is reduced to the lower limit of the annealing range.' The temperature gradient is so controlled that at the lower end of the annealing range, the center to surface gradient does not exceed 30 F. VYThe determination of the center to surface gradients in'glass have been'made by measuring the surface temperature. andthe mean temperature of the glass. These values are' utilized to calculate the temperature at the center of the. glass by means of differential equations whichV havebeenideveloped and which are not part of the present invention.. It is understood that the complete elimination of a temperature gradient ktlncmgh the thickness of the glass 'sheetfrom onegsurface to fthe other is not practical, especiallywhen an attempt is madeto draw thesheet upwardly from the molten bath' to Ya location wherein the optimum annealing temperature of Ythe glass is atf tained in' the shortest-'distance possible. However, by maintaining Vuuiform surface temperature from on'e'` side of theglass'sheet to the other on both surfaces thereof, thetask of providing a cooling etect on the` glass such that internal stresses tend to cause minimumwarpage and inhomogeneities of the glassis simplied',land the.

calculation ofthis optimum cooling curve for the various thicknesses of glasstobe .drawn may be accomplished with relativeiacility. Once this curve hasbeene'stabf lished, the problemof obtaining the proper 4adjustmentv ofthe various `thermoresponsive elements top rovide a proper cooling effect to 'the glass is readily accom plished. I Referring to Figures 6 and 7 a typical vhorizontalannealing lehr provided with temperature control elements for controlling the 'temperature "of a horizontally con# veyed glass ribbon 10 is shown. A plurality of conveyor rolls 100 areprovided to supportthe under surface of Y the horizontally conveyed glass ribbon 10. The rolls'conY vey'V the ribbonhorizontally through a :lrstV section of thejflehr where the temperature exceeds the annealing range ofthe glass, a secondsection of the lelir where l n the first section ofthe lehr, aplurality of differential coolers generally indicated at i s provided above and below therglass sheet. Differential coolers,115 are simi#A 1arte-the differential coolers 15 shown in ,themvertical annealing lehr'rand comprise' a series of Water cooled v v pipes or tubes 116 anda series of electrical heating elements 118. The'purpose ofthe dilerentialrcoolenll is, the same as that of differential cooler 15. Theam'ount b f'cur'rentsupplied'to heating elements 118 is controlled byfthermo-responsiveV elements trained on the temperature is within the annealingrang, and; liinally, section where the'temperature is'ibelow th e jajr1r V"contienenby; tnsenings 'finte yar'ionswnerm j f eagejporifio Drone sine 'f'thevenicliyldrawn-ihet; respectively, .andra similar arrangementftthermoffespon- Y neling rangefis'independent f he 'control 'orev'erjy ture is controlled, 'ftlrerve' are'V s'ix in'depedent lheing .Eir-

`cits 'for contrlling'the temperaturefofheglasspassing Vtota Lseties fofheat'ing Aelements byincnsV of l-saturlle,

:the g position fofj the second "horizontally ligned'rser'ies if thermo-responsive lements 32 -and 32. n

'11s. vColring' ply 21.45

i' l i upwardlylmi/ing- Ysheet V-erossesthe Y,temperelevel, the relay swtchSl is actuted therebyceusingcurrentftoowrnthe control circuit.V f j 'Y 4The current `Howl the control Vcircuit .ubalancesf the heating circuit, and lesscns :the Ieect f 'thechokeacoil n Y 51 oni-'the voltagebin'g TYsupplied to -theheating'c/irciiit from the source'EL An increasedfyoltage results-across A n the `'heating element .ISIunt/il :s'uc'h'tirne as fthe hezitlimY parted by 'the'heatng lernent causes :thetenjiperature' i inthe area-scanned-fby thejthermoresponsiyeelexnnt y Vcontrolled'independentlyof 4the Vother'sfbyvfthe surface temperature of .the glass .sheet Vat six-.different locations all ,at the Vsarneplarne,iand settingnthe individual .thermp- 5 Yresponsive elements controlling A'each he't'ing circuit't the -sarnei elevtionlrto. hesresponjs'ive aitv the rsaine telnr-YYV ,peraturefthe'temperature from sidelto side and between tionrof a-flat 'sheet of.window'glrarss.

One of the factors determiningtheoptimurrftenant:l l Y l i i'tur'e'forY annelringrthefising sheet ofig'lassismther'dinien Y sions oftheV vsheetY `Since the Y,Width fof rtheV drawn sheet is kept constantgihe onlyfyariahleigdimension thatneed tlireV o Vthe Aannealing@frarrige at -appolimately thetlevel -V locnlizedkeren alternating surfemffmspr '52. that ghfth heatingVA ,cils'ISl'contined Y ture 'yersursseleyzitionlevel the {ennelin'g sectionY l 'of 'the drawing machine that Y corresponds substantiallyl toY a1 theoretical cooling curi/'e1V designed Ato Y.produceV *2in1V i 'jwhirchnitv'is .drawn4 determine its( th'icltnerss's.` fGerieraiIly,v Y

'- .the :thickness varies .inverselygas Yet `lKoga,rithgrnic:f-ffunctio Vnaaking furnaces .my V'he increased. v

' fresponsiyejelement reactor'circnit-slinj each-'set of heting Y z v.circuits toprovidea uniforrfcoling Ycurve Voffteierag-n of the'speed ndfrteniperaturevof drauf. i; Byfrnpidlycooling vthevsheet irnmedilatelyabove,the'rnoltenbath,"a*sheet4V Y of n given thickness may beadrawn atiafmore'rapid rntef4 than has. beenpossiblefbefore; The rete of dran/has f beenallirnitng. Yfactor fin .the VYamountfot" Window:..g produced.; Q Henceljy proyidingi@aiV nleanslfforfacceler A ing the-rate of Jdraw, t'he productiyity ofV YuindoW glassl? by a.' relatively -rpid drW alt/verno I"areas" ofJ glass "surface i This current lheatsii'the 'flennts yf`1- 18 4'to `rn`odify"the c'o'olin'ge'ffect ofthe Vcoling "tub `sV ',116`in` theiirstsection of the "lehr, :In the" second section of the lehr,"when the glass ribbon jis coolejd tothe upperen'd of the' annealing Ir'an'ge, fslliicientadditional heat "is imparted 'by'means of additional: thermo-r'esponsive Velements 130 controlling add- .'tional `h'e'ating"elem`ents '118 Vtoprovfide nist, a minimization'lofjteinperatregradients' throughout the thickness vrof the 'glass sheet'at a`temperature"approximately equal to that' lof `the'upper "of ithe annealing range and l'sfecondly,vltoc'ontrol :the rate of cooling of the 'glass "thfough the annealing "range, ina "manner similar to vthatY des'cribed'previou'sly for thevertical lehr. AIn`'practice the heatingelements do'not'heat the glass. They niereiy' actas controllable the'rm'al'barriers by means of fwln'ch heat loss from the fglass visV accurately regulated.

The glassribbon'may'be 'cooledrap'idly in the third Vsection of thel horizontal `l'ehr,wher'e thefglass tempera- "belowthe annealing range 4of Vthenov'ing glass `s eet.

The V"cooling 't'ub'es '116 and heating elements 118 throughout the entire lehr are required tobe-so disposed iii/ith"respecttothe'upper and low'ensurfa'ces of the glass ribbonso "thatthe 'rate of cooling between opposite' glass surfacessinniforn Thus, the cooling enect f the i'o- 'itating 'conveyor l'rolls '100 'upon the temperature ofthe glass sheet must be taken intoV account in'loca'ting the cooling pipes 'and heating'elements above and below the 'glass sheet. v

'Byincr'ea'sing the 'rate of cooling of aribbon'offglass that isconv'eyed through an annealing lehr in theregions of the lehr where the temperature is above and below the annealing temperature'range for thegla'ssfthe length of the lehr lis substantially reduced. This reduction in {lehr length provides considerable economy in the operation of afglass plant, since space-is ata-premium in"m`ost `il-"glustrial establishments. Y

typical-structural assemblies Aof avertical and `a''hori- -zontal5annealing lehnembodyinga:plurality of 'check Vpoints for` conforming thejemperature-of a glass'sh'eetbr ribbontothe desired temperature required for atheo're'ticalcoolingcurve*as ,theglass passeseach'fcheckpoint have beenfdasribefl-u ,It vis understoodfhowever, that various imodiiicatiogiswofstrueture thatarereadily apparent 'to a mechanic skilled in Vvthe art willbecome obvious upon study of the present'disclos'ure. "The"scope of this inven- *tion should. notbe limited 'tothe specific details tfthe particular embodiment -descrvibedherein for purposes of illustration only'fbifsholbe eipanded to includethe "nattrirecitdfin the pperi'cled lirns. {The-"apparatus of my -iiiexitionfis clainied -'in `rny depending-divisional patent application, Serial No. 560,978, led January 24, 1956, and entitled Annealing Glass.

What is claimed is:

jgrasstiranni ene-acharne avan annealin'g'tenrperarnre s'bstantially at 'the upper-limitof the anne'aling'rn'ge for a suc'ient lengthY dirimere 'reduce substantially said temperature gradient, andrpassingthe ribbon throng-h an annealing zoneto`^'c"oolmesurfaces on bth 'sides of the glass ribbonata progressively increasingr'ate offcoolin'g while maintaining eqli'alization'ofV surface temperatures thereacrossY andbetween {he two sides, whereby the 'glass surfaces are simultaneously cooled to the lower limit of lthe annealing range and lthe temp'e'rature'gradient between the center and the jsu'rfac'es is increased in thefport'ion's thereacross by -a uniform amount.

l2. 'Apro'cess 'which 'comprises forming a continuous ribbon of glassfrom a' molten glass bath,"moving theglass ribbon through a cooling zone 'before the glass has'cooled to the annealing temperature range, passing 'huid coolant through the :cooling zonev on"each side 'of the moving glass ribbon in indirect heatvexchange relationship with the glass ribbon, Aelectrically heating 'separately VVportions of the coolingy zione opposite central and anking portions of the glass surface Lacross the ribbon and on cach side thereof within the cooling zone, maintaining said electrical heating of each ofsaid portions, separately adjusting the amount of electrical heating of veach Vof said portions,

. lwhereby the central andvflan'king portions of the surface of the glass 'ribbon on-'each side are cooled rapidly Vto Vreach an Vrannealing 4temperature vsubstantially at the upper limit of the .annealing frange,v at substantially the same vvtime and' toI create a temperature gradient between the center ofthe v'glass 'and thesurfaces that is substantially uniform inthe portionsY of Athe glassY ribbon, passing the cooled ribbonfthrou'gh 'an equalizing zone while maintaining 4the: central and "flanking portions of the surface of the glass -lribbon oneach sideat an annealing temperaterre 'substantially at'ftheupper limit A'of 'the annealing -rangefor afsii'cient lengthoftir'neto reducesubstantially vsaid tempeature gradienn'and Y'passinglthe ribbon through rranneling zone-to-cool'theisurfaces on both'fsides of Vvthe lglassribbbn atlalprogr'essi-vely increasing rate=of coolin'g Vwhil'emaintaining"equalization of surfacetemperaturesthereacross and betiv'een'the'twosides, wherebythe -glasssrfacesarelsihiultaneously cooled tothe lower `limit of v`4the4 annealing-"range land lthe Vtemperature fgra'dient 'between -th'e center-a'ndy the-surfaces 'is increased inl the paniere ther frees-ny' fa enfermement.

t `-the glas rlib'bo upwardly-'through ai cooling zonebefore 1. A process which comprises forming a continuous Y ribbon of glass from a molten glass bath, moving the glass ribbon through a cooling zone before the glassV has cooled to the annealing temperature range, passing fluid coolant through the cooling zone on each side of the moving glass ribbon in indirect heat exchange relationship with the glass ribbon, applying heat separately to portions of the cooling zone opposite portions of the glass surface across the ribbon and on each side thereof within the cooling zone, maintaining said application of heat to each of said portions, separately adjusting the amount of said heat application to each of said portions, whereby the por- Y tonsof the surface of the glass ribbon on each side are cooled rapidly to reach an annealing temperature substantially at the upper limit of the annealing range at substantially the same time and to create a temperature gradient between the center of the glass and the surfaces that is substantially uniform in the portions of the glass ribbon, passing the'cooled ribbon through an equalizing zone while maintaining the portions of the surface of the theFg'lsslhas cooled tothe1nnealingtemperature' range, fpassing iwater' through'lthefcooling :zone on each.' side Vof the fmoving glass ribbon'in zindirect -heat exchange frela- `tionship-ivithfthe: glass xribbonfelectrically heating separately portions of the cooling zone opposite central and flanking portions of the glass surface across the ribbon and on each side thereof within the cooling zone, maintaining said electrical heating of each of said portions, separately adjusting the amount of electrical heating of each of said portions, whereby the central and anking portions of the surface of theglass ribbon on each side are cooled rapidly to reach an annealing temperature subl stantially at the upper limit of the annealing range at substantially the same time and to create a temperature gradient between the center of the glass and the surfaces that is Vsubstantially uniform in the portions of the glass ribbon, passing the cooled ribbon upwardly through anV equalizing zone while maintaining the central and anking portions of the surface of the glass ribbon on eachV side at an annealing temperature substantially at the upper limit of the annealing range for a sufficient lengthof time to reduce substantially said temperature gradient and between the two sides, whereby-the glass surfaces are:

simultaneously cooled to the lower -limit of the-annealing range and the temperature gradient between the center and the surfaces is increased in the portionsthereacross of the glass surface across the ribbon andon eachrside thereof within the cooling zone, said radiant Yenergy in each of said portions being directed toward the glass ribbon, measuring separately infrared radiation from each of said portions of the surfaces of the glass ribbon, separatelyV controlling Vthe amount of radiant energy being directed toward each portion of Vsaid glass surfaces in response to the measured amount of infraredradiation from each of said portions of the glass surfaces, whereby the portions of the surface of the glass ribbon on each side are cooled rapidly to reach an annealing temperature substantially at the upper limit of the annealing range at substantially the same time and to create a temperature gradient between the center of the glass and the surfaces that is/Vsubstantially uniform in the portions of the glass ribbon, passing the cooled ribbon Vthrough an equalizing zone while maintaining the portions of the surface ofthe glass ribbon on each side at an annealing temperature substantially at the upper'limit of the annealing range for a sufcient length of time to reduce substantially said temperature gradient, and passing the ribbonrthrough an annealing zone to cool the surfaces on both sides of Vthe glass ribbon at a progressively increasing rate of cooling while maintaining equalization of surfacel temperatures thereacross and between the two sides, whereby the glass surfaces are simultaneously cooled tothe lower limit of Vthe annealing range and the temperature gradient between heating said portions of the zone oppositeV said central 12 and tlanking portions, said'tradant energy in each of said portions being directed toward `the glass ribbon, measur'- ing separately infrared'radia'tion from each of said portions of the surfaces of the glass ribbon, separatelycontrolling the amount of electrical-heatingfor each portion of the zone in response to lthe measured amount ofY infrared radiation from each of said opposite portions of the glass surfaces, whereby-thecentral and flanking portions of the surface of the glass ribbonon each s'idef arecooled rapidlyrto.` reach anannealing temperaturesubstantially Vat the upper limitv of the annealingV range atsubstantially the same time'and tofcreate artemperature gradientbetween the center of the glass 'and the vsurfaces that issubstantially uniform in the portions of theglass ribbon, passing the cooled ribbon through `an ,equalizing zone while maintaining the central and lankingv portionsA ofthe surface of the glass ribbon on eachlsidetatran annealing temperature substantially at theV upperl limitof the anneal-V ingrange for a suicientlength of time to reducesubstan` Y tially said temperature gradient, and passing-thezribbo'n f through an annealing zone to Vcool the surfaces onbth, sides of the glass ribbon ata progressively increasing rate of cooling while maintaining equalization Yof surface temperatures thereacross and between the two sides, whereby the glass surfaces are substantially cooled to the lower limit of the annealing range and the ternperaturefgradient between the center and the surfaces is Vincreased inthe portions thereacross by a uniform amount.

6. The process of claim 5 whereinthe step of forming a continuous ribbon is forming said ribbon'vertically,

wherein the glassribbon is moved upwardly through the cooling zone and wherein the fluid coolantis water.,

References Cited in the file of this patent Handbook of kGlass Manufacture,'Tooley. by Ogden Publ. Co., New York-1953, pages 398-490. 

